RAM Structural System Help

Stress and Force Contours

The program stores forces and stresses for walls/diaphragms during analysis if the option to store wall/diaphragm stresses and internal forces is selected before analysis is started (see Criteria – General – Wall/Diaphragm). These results can be displayed on structure by invoking Process - Results - Stress and Internal Force Contours menu command (also it is available in the toolbar).

Stresses are normal, shear and out-of-plane (transverse) stresses and they are expressed as force per unit area. They are first calculated at shell integration points and then, they are extrapolated to shell corner nodes. Shell stresses are calculated at both top/positive and bottom/negative faces.

Internal Forces (also known as shell resultants) are forces and moments resulted from integrating stresses over shell thickness. They are expressed as forces and moments per unit of in-plane length.

By default, stress/internal force values are averaged at nodes and contour plots are displayed accordingly. It is possible to show results per each shell element by not selecting Stress Averaging option in the Stress and Internal Force dialog. The option Show Stress contour values can be used to show stress\internal force values on screen (they always represent stresses/internal forces values calculated at shell nodes). In addition, it is possible to display stress/internal force on deformed shape for selected load case/combo (see the option Display on Deformed Shape).

It is important to note that averaged max/min values (such as SMax/SMin or FMax/FMin) are calculated from averaged values of S11, S22 and S12 (or F11, F22 and F12) at nodes.

In the following discussions, we refer to the following figure:

Stress and Internal Force Definitions

Wall and Diaphragm Stresses

Stresses displayed on screen are shown as force per unit area. They are acting on Top/Positive or Bottom/Negative face of shell element.

Table 1. Positive Definition of Stresses: In-Plane (force per unit area)
S11 Normal stress acting on positive and negative face 1 in the direction of axis 1
S22 Normal stress acting on positive and negative face 2 in the direction of axis 2
S12 Shear stress acting on positive and negative face 1 in the direction of axis 2
SMax Maximum principal normal stress 1
SMin Minimum principal normal stress 1
SVmax Maximum principal shear stress 2
Von Mises Von Mises principal stress 3
  1. Principal normal stresses are oriented in such a way that associated shearing stress is zero.
  2. Maximum principal shear stress is calculated as follows:
    S V m a x = A b s S M a x -   S m i n 2
    where
    S M a x , S m i n
    =
    principal maximum and minimum normal stresses, respectively
  3. Von Mises principal stress is calculated as follows:
    S V M =   S M a x 2 - S M a x S m i n + S M i n 2
    where
    S M a x , S m i n
    =
    principal maximum and minimum normal stresses, respectively
Table 2. Positive Definition of Stresses: Out-of-Plane-Shear (force per unit area)
S13 Out-of-plane shear stress acting on positive and negative face 1 in the direction of axis 3
S23 Out-of-plane shear stress acting on positive and negative face 2 in the direction of axis 3
SAvgMax Maximum out-of-plane shear stress1
  1. Maximum out-of-plane shear stress is calculated as follows:
    S V M =   S 13 2 + S 23 2
    where
    S 13 , S 23
    =

    out-of-plane stresses in the direction of axis on face 1 and 2, respectively.

Wall and Diaphragm Internal Forces

Internal Forces displayed on screen are shown as force per unit of in-plane length. They are acting at mid-surface of shell element.

Table 3. Positive Definition of Internal Forces: Membrane force (force per unit of in-plane length)
F11 Normal force acting at mid-surface on positive and negative face 1 in the direction of axis 1
F22 Normal force acting at mid-surface on positive and negative face 2 in the direction of axis 2
V12 Shear force at mid-surface acting on positive and negative face 1 in the direction of axis 2
FMax Maximum principal normal force acting at mid-surface1
FMin Minimum principal normal force acting at mid-surface1
Von Mises Von Mises principal force2
  1. Principal normal forces are oriented in such a way that associated shearing force is zero.
  2. Von Mises principal force is calculated as follows:
    F V M =   F M a x 2 - F M a x F m i n + F M i n 2
    where
    F M a x , F m i n
    =
    principal maximum and minimum normal forces, respectively
Table 4. Positive Definition of Internal Forces: Plate moment (moment per unit of in-plane length)
M11 Normal moment acting at mid-surface on positive and negative face 1 about axis 2
M22 Normal moment acting at mid-surface on positive and negative face 2 about axis 1
M12 Twisting moment at mid-surface acting on positive and negative face 1 about axis 1, and on face 2 about axis 2
MMax Maximum principal moment force acting at mid-surface1
MMin Minimum principal moment force acting at mid-surface1
  1. Principal moments are oriented in such a way that associated twisting moment is zero.
Table 5. Positive Definition of Internal Forces: Transverse shear (shear per unit in-plane length)
V13 Out-of-plane shear acting at mid-surface on positive and negative face 1 about axis 3
V23 Out-of-plane shear acting at mid-surface on positive and negative face 2 about axis 3
VMax Maximum principal shear1
  1. Maximum principal shear is calculated as follows:
    V M a x =   V 13 2 + V 23 2
    where
    V 13 , V 23
    =
    out-of-plane shears, respectively

Stress and Internal Force Contours on Wall and Diaphragm

Stresses and internal forces are direction dependent quantities. They are portrayed graphically according to local axes of walls and diaphragms. Local axes of walls and diaphragms are defined as follows (in the following descriptions, right-hand-rule is adapted and, local axes 1, 2 and 3 are perpendicular to each other):

Wall

Local axis 1 and 2 are on plane of wall and local axis 3 is perpendicular to plane of wall. Local axis 2 is always oriented along global axis Z (also note that e2 = e3 x e1). Top (or positive) face of wall is in the direction of positive local axis 3.

Diaphragm with Composite Floor Deck/Slab

If the option Apply Stiffness Modification Factors is selected (see Deck/Slab Property Information dialog in RAM Manager), local axis 1 is in the direction of deck orientation. Local axis 3 is perpendicular to plane of deck. Local axis 2 is constructed from other axes as follows: e2 = e3 x e1.

If the option is not selected, local axes 1, 2 and 3 are in the direction of global axes X, Y and Z, respectively. Top (or positive) face of diaphragm is in the direction of positive local axis 3.

Diaphragm with Noncomposite Floor Deck/Slab

If the option Apply Stiffness Modification Factors is selected (see Deck/Slab Property Information dialog in RAM Manager), local axis 1 is either in the direction of deck orientation (if deck is one-way) or it is defined at user-defined angle measured from global axis (if deck is two-way). Local axis 3 is always perpendicular to plane of deck. Local axis 2 is constructed from other axes as follows: e2 = e3 x e1. If the option is not selected, local axes 1, 2 and 3 are in the direction of global axes X, Y and Z, respectively. Top (or positive) face of diaphragm is in the direction of positive local axis 3.

Diaphragm with Concrete Slab

If the option Stiffness Modifiers is selected (see Deck/Slab Property Information dialog in RAM Manager), local axis 1 is either in the direction of deck orientation (if deck is one-way) or it is defined at user-defined angle measured from global axis (if deck is two-way). Local axis 3 is always perpendicular to plane of deck. Local axis 2 is constructed from other axes as follows: e2 = e3 x e1.

If the option Crack Factors is selected, local axes 1, 2 and 3 are in the direction of global axes X, Y and Z, respectively. Top (or positive) face of diaphragm is in the direction of positive local axis 3.

(a) (b)

Local axes definitions of (a) wall and (b) diaphragm (global setting shown)